Early predictions that a spin-polarized current can apply a torque on DW have since opened the possibility for various forms of current controlled spin texture motion,[1]} laying the groundwork for the burgeoning field of spin texture-based memory and computing applications. Spin textures are traditionally driven by spin transfer torque (STT),[2]} wherein their motion is induced by the transfer of spin angular momentum, albeit at modest velocities using relatively high current densities. [3]}, [4]} The discovery of spin orbit torque (SOT), arising from spin Hall [5]}, [6]} and Rashba-Edelstein [7]}, [8]} effects, enables the generation of larger in-plane spin currents per electron charge at HM/FM interfaces. [6]}, [10]} Consequently, superior switching speed is enabled by the exertion of such in-plane torque on the perpendicular magnetization over nanosecond timescales, [11]} making SOT an increasingly attractive instrument for the electrical manipulation of chiral spin textures with ultrafast dynamics[12]}, [13]}, [14]}, [15]}.
